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Volumn 53, Issue 5, 1996, Pages 2998-3013

Discrete Wigner function and quantum-state tomography

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EID: 4244098305     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.53.2998     Document Type: Article
Times cited : (213)

References (111)
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    • (Springer, Berlin, 1980) raised the question whether the wave function can be reconstructed from position and momentum distributions. The general problem of state reconstruction was stated by
    • A look at the history of the quantum-state measurement schemes may be interesting. W. Pauli, General Principles of Quantum Mechanics (Springer, Berlin, 1980) raised the question whether the wave function can be reconstructed from position and momentum distributions. The general problem of state reconstruction was stated by U. Fano, Rev. Mod. Phys. 29, 74 (1957).
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    • Strictly speaking, the presented formalism is only valid for odd-dimensional systems. However, it can be easily extended to even-dimensional ones using the theory developed here and in Ref. 11
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    • Quantum control schemes can be used to create arbitrary states of Zeeman multiplets. This is a necessary ingredient in the quantum-state synthesis via adiabatic passage by A. S. Parkins, P. Marte, P. Zoller and H. J. Kimble, Phys. Rev. Lett. 71, 3095 (1993).
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    • J. F. Clauser and J. P. Dowling (unpublished) for an analogue in classical optics. A d-period diffraction grating represents the spin system and the classical propagation of light plays the role of the precession
    • J. F. Clauser and J. P. Dowling (unpublished) for an analogue in classical optics. A d-period diffraction grating represents the spin system and the classical propagation of light plays the role of the precession.
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    • N. M. Korobov, Trigonometricheskie summy i ikh prilozhenia (Nauka, Moscow, 1989), Sec. 3. Sums of the type (88) are called Gauss sums. See also Ref. 33
    • N. M. Korobov, Trigonometricheskie summy i ikh prilozhenia (Nauka, Moscow, 1989), Sec. 3. Sums of the type (88) are called Gauss sums. See also Ref. 33.


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